CN211014017U - Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system - Google Patents

Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system Download PDF

Info

Publication number
CN211014017U
CN211014017U CN201921894219.5U CN201921894219U CN211014017U CN 211014017 U CN211014017 U CN 211014017U CN 201921894219 U CN201921894219 U CN 201921894219U CN 211014017 U CN211014017 U CN 211014017U
Authority
CN
China
Prior art keywords
light
sample
coaxial transmission
total reflector
device suitable
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn - After Issue
Application number
CN201921894219.5U
Other languages
Chinese (zh)
Inventor
潘凌云
屠宏宇
黄晓丽
黄艳萍
崔田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Jilin University
Original Assignee
Jilin University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Jilin University filed Critical Jilin University
Priority to CN201921894219.5U priority Critical patent/CN211014017U/en
Application granted granted Critical
Publication of CN211014017U publication Critical patent/CN211014017U/en
Withdrawn - After Issue legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

The utility model relates to a coaxial transmission-type transient state absorption measuring device suitable for superhigh pressure microcavity system belongs to high-pressure device microcavity system and measures the field. The method comprises the following steps: the device comprises a femtosecond pulse laser, an optical parametric oscillator, a monochromator, a photomultiplier signal receiving device, a lock-in amplifier, a CCD display, a cold light source, a reflector, a convex lens, a spectroscope, a long-working-distance microscope objective, a lens group, a sample cell and the like. Has the advantages that the structure is novel: by combining the photomultiplier, the phase-locked amplifier and the long-working-distance microscope objective, the signal-to-noise ratio of the system is greatly optimized, the sensitivity can be less than 0.00005, and the device is suitable for high-voltage systems under extreme conditions. And a coaxial pump detection laser detection mode is adopted, so that two light lasers can enter the sample cavity and can be ensured to receive detection light. The system adopts a cold light source to provide illumination, so that the sample cavity is illuminated, the sample cavity can be visible on a display, and the laser can accurately detect the required sample.

Description

Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system
Technical Field
The utility model belongs to the technical field of high pressure device microcavity system measures, especially indicate a coaxial transmission-type transient state absorption measuring device of superhigh pressure microcavity system.
Background
At present, ultrafast dynamic detection light path means are mature, but only some samples with stronger absorption signals can be selected for a sample to be detected, and for samples with weaker signals, the signals of the samples cannot be accurately detected due to the poorer signal-to-noise ratio of a system. With the development of high pressure technology, the need for detecting optical properties of substances under high pressure has increased, including the study of time-resolved transient absorption of substances.
However, under extreme conditions the signal of the sample will gradually decrease such that the conventional detection system cannot detect the signal of the sample at the ultra-high pressure. And because the device that produces the high pressure is sealed the sample in the sample chamber that only has hundreds of microns, even several microns, the cross pump detection that is commonly used at present is not applicable to high pressure device, moreover because the sample is less, and the intracavity still mixes the marking ruby, so still need the sample chamber visual, just can guarantee that the pump detects the laser and can detect the sample.
Disclosure of Invention
The utility model provides a coaxial transmission-type transient state absorption measuring device suitable for superhigh pressure microcavity system to the signal of solving sample under extreme condition can weaken gradually, so that ordinary detecting system can not detect the problem of the sample signal under the superhigh pressure.
The utility model adopts the technical proposal that: a beam of laser generated by the femtosecond laser is divided into two beams of light by the first spectroscope through the first total reflector and the second total reflector, wherein one beam of light is incident to the hollow retroreflector fixed on the electric translation stage through the third total reflector and the frequency doubling crystal and is emitted from the hollow retroreflector, so that the emergent light and the incident light are completely parallel and in the same plane, and then reach the optical climbing frame through the chopper, the fourth total reflector and the second spectroscope;
the other beam of light split by the first beam splitter passes through a fifth total reflector, a sixth total reflector and a seventh total reflector, the beam of light is converged to a nonlinear material by the first convex lens to obtain super-continuous white light covering the whole visible light wave band, the super-continuous white light is converged by the second convex lens, and the converged light reaches the optical climbing frame through the eighth total reflector and the second beam splitter;
two beams of light reaching the optical climbing frame are in a coaxial state, and enter the pressurizing device through the third spectroscope and the long-working-distance microscope objective, a sample is arranged in a sample cavity of the pressurizing device, emergent light passes through the lens group and is converged by the third convex lens, then a monochromator receives a light signal, the signal is amplified by the photomultiplier tube, a phase-locked amplifier separates out a required carrier frequency signal, and the carrier frequency signal is output;
the sample chamber visualization system is: the cold light source provides illumination light, the illumination light reaches the sample stage through the movable total reflection mirror and the lens group, the sample chamber is illuminated, the light is reflected by the third spectroscope through the long-working-distance microscope objective lens, the fourth convex lens, the image is transmitted to the CCD receiver through the fourth convex lens, and then the image is displayed on the CCD display.
The nonlinear material of the utility model comprises sapphire and calcium fluoride.
The femtosecond laser produces femtosecond laser's wavelength and is 800nm, and repetition frequency 1KHz becomes 400nm after the doubling of frequency.
The movable full-reflecting mirror is composed of a full-reflecting mirror and a movable base.
The chopper adopts an external trigger mode.
The utility model has the advantages that: firstly, through the combination of a photomultiplier, a phase-locked amplifier and a long working distance microscope objective, the signal-to-noise ratio of the system is greatly optimized, the sensitivity can be less than 0.00005 (five hundred thousandths), and the sensitivity is far lower than that of a common device, so that the system can detect a sample signal which is weak under pressure, and is suitable for a high-pressure system under extreme conditions. A coaxial pump detection laser detection mode is adopted, so that two light lasers can enter a sample cavity no matter how small the size of the sample cavity is, and the detection light can be received. The system adopts a cold light source to provide illumination, illuminates the sample cavity and then enables the sample cavity to be visible on a display through a CCD receiving device, so that the problems of the existing detection system are solved, and the laser can be ensured to accurately detect the required sample.
Drawings
Fig. 1 is a schematic diagram of the optical path of the present invention;
FIG. 2 is a schematic diagram of the interior of a conventional high-voltage apparatus;
FIG. 3 is an image of a perylene sample on a CCD imaging device in a high pressure device when not pressurized;
FIG. 4 is an image of a perylene sample on a CCD imaging device in a high pressure device with the perylene sample pressed to a near transparent ruby;
FIG. 5 is a graph of transient absorption spectra of a sample perylene under different pressures in a high pressure device;
fig. 6 is a graph of the signal-to-noise ratio of the absorption spectrum under extreme pressure in a high voltage device.
Detailed Description
A beam of laser generated by the femtosecond laser 1 is divided into two beams of light by a first beam splitter 4 through a first total reflector 2 and a second total reflector 3, wherein one beam of light is incident to a hollow retroreflector 7 fixed on an electric translation stage 8 through a third total reflector 5 and a frequency doubling crystal 6 and is emitted out of the hollow retroreflector, so that the emergent light and the incident light are completely parallel and in the same plane, and then reach an optical climbing frame 19 through a chopper 9, a fourth total reflector 10 and a second beam splitter 18;
the other beam of light split by the first beam splitter 4 passes through a fifth total reflector 11, a sixth total reflector 12 and a seventh total reflector 13, the beam of light is converged to a nonlinear material 15 by a first convex lens 14 to obtain super-continuous white light covering the whole visible light wave band, the super-continuous white light is converged by a second convex lens 16, and the converged light reaches an optical climbing frame 19 through an eighth total reflector 17 and a second beam splitter 18;
the two beams of light reaching the optical climbing frame 19 are in a coaxial state, and enter the pressurizing device 22 through the third beam splitter 20 and the long-working-distance microscope objective 21, a sample is arranged in a sample cavity of the pressurizing device, emergent light passes through the lens group 23 and is converged by the third convex lens 25, a monochromator 27 receives a light signal, the signal is amplified by the photomultiplier 29, a required carrier frequency signal is separated by the phase-locked amplifier 30, and the carrier frequency signal is output; it is transmitted to any of the computers 26.
The sample chamber visualization system is: the cold light source 28 provides illumination light, the movable total reflection mirror 24 is pushed to the position of the dotted line from the position of the solid line shown in the figure, the illumination light reaches the sample stage 22 through the movable total reflection mirror 24 and the lens group 23, the sample chamber is illuminated, the long working distance microscope objective 21 is used, the third spectroscope 20 reflects the light to the fourth convex lens 31, the image is transmitted to the CCD receiver 32 through the fourth convex lens, and then the image is displayed on the CCD displayer 33.
The nonlinear material 15 of the present invention comprises sapphire and calcium fluoride.
Femtosecond laser 1 produces femtosecond laser's wavelength and is 800nm, 1KHz is had a repetition frequency, becomes 400nm after the doubling of frequency.
The optical electric translation stage 8 and the hollow retroreflector 7 form a translation stage system, and the hollow retroreflector is used for keeping incident light and emergent light parallel and finally moving according to requirements through computer control.
The cold light source 28, the CCD receiver 32 and the CCD display 33 form a CCD imaging system, the cold light source enters the monochromator through the movable total reflector and enters the CCD receiver through the lens group from the back side of the high-voltage device, emergent light enters the CCD receiver through the long-working-distance microscope objective, the spectroscope and the fourth convex lens, and the CCD display images the sample in the device and the position excited by laser.
Portable total reflection mirror comprises total reflection mirror and portable base, switches convenient and practical in order to can be with total reflection mirror at lighting system and test system.
Chopper 9 adopt the mode of triggering outward, need not all adjust the chopping frequency at every turn, can change the chopping frequency through the repetition frequency of laser instrument is automatic, this kind of chopping mode is convenient and fast more, is different from the free chopping mode of traditional chopper.
The signal amplification system is composed of a long working distance microscope objective lens 21, a photomultiplier 29 and a phase-locked amplifier 30.
The pressing system in a high pressure device is a pair of diamond anvils with anvil faces of hundreds or even microns in diameter. A hollow steel sheet is placed between the anvil faces and serves as a sample cavity, and the radius of the hollow part is smaller than half of that of the diamond anvil face. Therefore, the light-passing aperture corresponding to the sample cavity is 1/10 to 1/100 of the normal-pressure light path, the light path needs to be introduced into the sample cavity by means of a microscope objective, and after an optical signal is received by a monochromator, the signal needs to be amplified by a photomultiplier because the signal is very weak, and then the signal is integrated and weakened by noise through a phase-locked amplifier and then can be output to a computer.

Claims (5)

1. A coaxial transmission type transient absorption measuring device suitable for an ultrahigh pressure microcavity system is characterized in that: a beam of laser generated by the femtosecond laser is divided into two beams of light by the first spectroscope through the first total reflector and the second total reflector, wherein one beam of light is incident to the hollow retroreflector fixed on the electric translation stage through the third total reflector and the frequency doubling crystal and is emitted from the hollow retroreflector, so that the emergent light and the incident light are completely parallel and in the same plane, and then reach the optical climbing frame through the chopper, the fourth total reflector and the second spectroscope;
the other beam of light split by the first beam splitter passes through a fifth total reflector, a sixth total reflector and a seventh total reflector, the beam of light is converged to a nonlinear material by the first convex lens to obtain super-continuous white light covering the whole visible light wave band, the super-continuous white light is converged by the second convex lens, and the converged light reaches the optical climbing frame through the eighth total reflector and the second beam splitter;
two beams of light reaching the optical climbing frame are in a coaxial state, and enter the pressurizing device through the third spectroscope and the long-working-distance microscope objective, a sample is arranged in a sample cavity of the pressurizing device, emergent light passes through the lens group and is converged by the third convex lens, then a monochromator receives a light signal, the signal is amplified by the photomultiplier tube, a phase-locked amplifier separates out a required carrier frequency signal, and the carrier frequency signal is output;
the sample chamber visualization system is: the cold light source provides illumination light, the illumination light reaches the sample stage through the movable total reflection mirror and the lens group, the sample chamber is illuminated, the light is reflected by the third spectroscope through the long-working-distance microscope objective lens, the fourth convex lens, the image is transmitted to the CCD receiver through the fourth convex lens, and then the image is displayed on the CCD display.
2. The coaxial transmission type transient absorption measurement device suitable for the ultrahigh-pressure microcavity system according to claim 1, wherein: the nonlinear material comprises sapphire and calcium fluoride.
3. The coaxial transmission type transient absorption measurement device suitable for the ultrahigh-pressure microcavity system according to claim 1, wherein: the wavelength of the femtosecond laser generated by the femtosecond laser is 800nm, the repetition frequency is 1KHz, and the wavelength is 400nm after frequency multiplication.
4. The coaxial transmission type transient absorption measurement device suitable for the ultrahigh-pressure microcavity system according to claim 1, wherein: the movable total reflection mirror is composed of a total reflection mirror and a movable base.
5. The coaxial transmission type transient absorption measurement device suitable for the ultrahigh-pressure microcavity system according to claim 1, wherein: the chopper adopts an external triggering mode.
CN201921894219.5U 2019-11-05 2019-11-05 Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system Withdrawn - After Issue CN211014017U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201921894219.5U CN211014017U (en) 2019-11-05 2019-11-05 Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201921894219.5U CN211014017U (en) 2019-11-05 2019-11-05 Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system

Publications (1)

Publication Number Publication Date
CN211014017U true CN211014017U (en) 2020-07-14

Family

ID=71480837

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201921894219.5U Withdrawn - After Issue CN211014017U (en) 2019-11-05 2019-11-05 Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system

Country Status (1)

Country Link
CN (1) CN211014017U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110609013A (en) * 2019-11-05 2019-12-24 吉林大学 Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110609013A (en) * 2019-11-05 2019-12-24 吉林大学 Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system
CN110609013B (en) * 2019-11-05 2024-03-01 吉林大学 Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system

Similar Documents

Publication Publication Date Title
CN110609013B (en) Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system
CN113740307B (en) Multi-mode nonlinear microscopic imaging system
CN207300872U (en) High time-space resolution transient state absorption spectrometer imaging system based on inverted microscope
CN211014017U (en) Coaxial transmission type transient absorption measuring device suitable for ultrahigh pressure microcavity system
CN109060150B (en) Ultra-short pulse time width measuring device and method based on spectral interference
CN115684079A (en) Transient absorption spectrum measuring system with high sensitivity and high signal-to-noise ratio
CN114839145A (en) Laser damage analysis test instrument
CN201273880Y (en) Apparatus for nondestructively testing doping concentration of laser crystal
CN112285036A (en) Frequency-reducing synchronous ultrafast transient absorption test system
CN117783013A (en) Imaging system and method for transient fluorescence and photocurrent
CN110596073B (en) Total reflection type femtosecond stimulated Raman spectrometer
JP2017067613A (en) Inspection device and inspection method
CN110274885B (en) Broadband time-resolved absorption spectrum single measurement device
CN106404695B (en) Spectrophotometer
CN208076388U (en) A kind of Terahertz detection device
CN216361769U (en) Heavy metal detection system of single laser source, three-pulse LIBS and fluorescence spectrum
CN210863540U (en) Rhodamine detection device based on fluorescence spectrum characteristics
CN114813648A (en) Heterodyne detection spontaneous Rayleigh Brillouin scattering spectrum method and device
CN102269716A (en) Test method for optical damage of microzone, and apparatus thereof
CN217638674U (en) High-flux nanosecond transient absorption spectrum measuring system
CN109238964B (en) Sensing device
CN209927718U (en) Remote measurement device based on fluorescence technology
CN105136329A (en) CARS (Coherent Anti-stokes Raman Spectroscopy) spectrum temperature measurement experimental device based on bifocal lens
CN221405372U (en) Laser detection system
CN112903624B (en) Terahertz biological detection method and device based on five-energy-level Reedberg quantum state

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant
AV01 Patent right actively abandoned

Granted publication date: 20200714

Effective date of abandoning: 20240301

AV01 Patent right actively abandoned

Granted publication date: 20200714

Effective date of abandoning: 20240301

AV01 Patent right actively abandoned
AV01 Patent right actively abandoned